Alpha-Absorption Lab Homework: Determining Geiger Counter Window Thickness

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SUMMARY

The discussion focuses on determining the combined thickness of a Geiger counter window and its protective coating by analyzing the counting rate of alpha particles emitted from a 241Am source. The experiment involves placing the Geiger counter in a plastic enclosure and measuring the counting rate with varying thicknesses of mylar sheets. Key calculations include using the stopping power of materials such as glass, air, and mylar, along with the energy of the alpha particles (5.48 MeV) to derive the necessary thickness measurements. Participants emphasize the importance of dimensional analysis in solving the problem.

PREREQUISITES
  • Nuclear physics principles related to alpha particle interactions
  • Understanding of stopping power calculations in materials
  • Dimensional analysis techniques for physical equations
  • Familiarity with Geiger counter operation and measurement techniques
NEXT STEPS
  • Research stopping power values for various materials, including glass and mylar
  • Learn about dimensional analysis in the context of nuclear physics
  • Explore the properties and applications of Geiger counters in radiation detection
  • Study the energy loss mechanisms of alpha particles in different media
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Students and educators in nuclear physics, laboratory technicians working with radiation detection, and researchers involved in experimental physics related to alpha particle measurements.

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Homework Statement



"Place the geiger counter in the plastic 241Am alpha-source enclosure. (basically, a distance of air separates the geiger counter window and the 241Am source) Re-apply the voltage and determine the counting rate. Repeat with various numbers of very thin mylar sheets on top of the source. The alpha particles of 241Am have an energy of 5.48 MeV. This information and a graph of counting rate versus absorber thickness may be used to determine the combined thickness of the Geiger counter window and any portective coating on the surface. To do this you will have to estimate the thickness of air between the source and the holder. A table of the rate of energy loss of alpha-particles of a variety of energies and materials is appended. It lists the energy per nucleon and the energy of alpha-particles."

Homework Equations



Nuclear physics knowledge and error analysis

The Attempt at a Solution



thickness of glass x stopping power of glass = Sigma (thickness x stopping power of the Am)? - thickness of air x stopping power of the air -thickness of mylar x stopping power of Mylar?

Ok I think I'm suppose to use the Energy/(mass/Area) for stopping power, but what what am I suppose write for Sigma (thickness x stopping power of Am)?
 
Last edited:
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YES YES YES, I figured it out after a lot of thinking, but only a little dimensional analysis:

Density glass x Length glass x Stopping power glass = Energy Am – Density N x Length Air x Stopping power N – Density O x Length Air x Stopping power O

(Length in cm, Stopping power in mg/cm2, Density in mg/cm3)
 
Now I just need to know stopping power of glass, anyone??
 

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